Higher-Spin Witten Effect and Two-Dimensional Fracton Phases

TL;DR

We study generalized $\theta$ terms in three-dimensional $U(1)$ higher-spin tensor gauge theories that host gapless higher-spin modes and fracton excitations. The bulk $\theta$ terms leave the gapless modes intact while binding electric to magnetic charges in higher-rank Witten-effect patterns, with rank-2 theories yielding distinct $\theta$-term classes, quantization, and time-reversal constraints. On boundaries, these terms induce tensor Chern-Simons theories that realize two-dimensional fracton phases, including both chiral and non-chiral varieties, and can realize fully 2D fracton physics under appropriate conditions. Together, the bulk–boundary structure reveals a pathway to tensor CS theories and 2D fracton phases, with generalized Hall responses that may be observable in suitably engineered systems.

Abstract

We study the role of "$θ$ terms" in the action for three-dimensional $U(1)$ symmetric tensor gauge theories, describing quantum phases of matter hosting gapless higher-spin gauge modes and gapped subdimensional particle excitations, such as fractons. In Maxwell theory, the $θ$ term is a total derivative which has no effect on the gapless photon, but has two important, closely related consequences: attaching electric charge to magnetic monopoles (the Witten effect) and leading to a Chern-Simons theory on the boundary. We will find that a similar story holds in the higher-spin $U(1)$ gauge theories. These theories admit generalized $θ$ terms which have no effect on the gapless gauge mode, but which bind together electric and magnetic charges (both of which are generally subdimensional) in specific combinations, in a higher-spin manifestation of the Witten effect. We derive the corresponding Witten quantization condition. We find that, as in Maxwell theory, imposing time-reversal invariance restricts $θ$ to certain discrete values. We also find that these new $θ$ terms imply a non-trivial boundary structure. The boundaries host fracton excitations coupled to a tensor $U(1)$ gauge field with a Chern-Simons-like action, in both chiral and non-chiral varieties. These boundary theories open a door to the study of $U(1)$ fracton phases described by tensor Chern-Simons theories, not only on boundaries of three-dimensional systems, but also in strictly two spatial dimensions. We explicitly work through three examples of bulk and boundary theories, the principles of which can be readily extended to arbitrary higher-spin theories.

Figures (4)

• Figure 1: When $\theta=0$, the set of possible charges forms a simple square lattice in the $(q,g)$ plane. (Adapted from Reference chong.)
• Figure 2: When $\theta$ is nonzero, the charge lattice is tilted. The case $\theta=\pi$ is seen above. (Adapted from Reference chong.)
• Figure 3: The $\theta_2$ term serves the purpose of attaching an angular configuration of electric charge (red) to the magnetic charge (blue).
• Figure 4: When $\theta$ is nonzero, electric fractons will be attached to the endpoints of the magnetic charge vectors. Due to the finite gap to electric charges, it will be energetically favorable for the magnetic charges to bind into string-like objects.